Internal Forces and Their Influence on the Earth's Surface

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Internal Forces and Their Influence on the Earth's Surface EARTH SYSTEM: HISTORY AND NATURAL VARIABILITY – Vol. I - Internal Forces and Their Influence on the Earth’s Surface - Plašienka D. INTERNAL FORCES AND THEIR INFLUENCE ON THE EARTH'S SURFACE Plašienka D. Slovak Academy of Sciences, Bratislava, Slovakia Keywords: Earth’s mantle, convection currents, lithosphere, strength, plate tectonics, tectonic forces, stress in the lithosphere, deformation, earthquakes Contents 1. Introduction 2. The Earth’s Interior—Thermal and Compositional Structure 2.1. Internal Heat 2.2. Geospheres 3. The Mantle Engine 3.1. Short-Term Mantle Properties 3.2. Convective Flow Patterns 4. Rheology of the Lithosphere 4.1. Flow Conditions 4.2. Brittle Behavior 4.3. Ductile Behavior 4.4. Layered Lithosphere 5. Stress in the Lithosphere and its Relaxation 5.1. Forces and Stresses 5.2. Stress versus Strain 5.3. The Brittle Crust and Seismicity 6. Conclusion Acknowledgments Glossary Bibliography Biographical Sketch Summary UNESCO – EOLSS Earth works like a heat machine, in which heat is transported from its interior towards the surface. This is the principal way Earth cools. The internal thermal and gravitational instabilities vanish due to mass movements that transport heat by thermal convection, mainly within Earth’sSAMPLE mantle. Increasing temp CHAPTERSerature lowers the rock strength so that rocks in Earth’s interior are able to flow in a viscous manner. Convection currents in the mantle ultimately induce various kinds of deformation and movements of the Earth’s upper layers. The stiff outer shell of Earth, the lithosphere, has a different composition and properties in oceanic and continental areas. The oceanic lithosphere is relatively uniform and strong, while the continental lithosphere, and especially its crust, is weak due to compositional and rheological layering. Consequently, the continental crust is prone to extensive deformation expressed by mountain building and seismicity. ©Encyclopedia of Life Support Systems (EOLSS) EARTH SYSTEM: HISTORY AND NATURAL VARIABILITY – Vol. I - Internal Forces and Their Influence on the Earth’s Surface - Plašienka D. The system of driving and resistive forces produces various stress fields in the lithosphere. Provided the rock strength is overcome, the stress is relaxed by deformation. Faulting, folding, and ductile creep are the main processes by which crustal rocks are deformed. Ductile flow in deeper parts of the crust initiates stress amplification in the brittle upper crust that is transiently relieved by seismic slipping along active faults, generating sometimes catastrophic earthquakes. 1. Introduction Earth’s surface, on which humankind lives, exhibits an endless variability in morphological forms. The continental exteriors vary from mountain belts and volcanic chains to hilly areas and flat lowlands, the oceanic bottom rises from large abyssal plains to seamounts and ridges and falls to narrow trenches. All this variability is an expression of the ever-present competition of two classes of energetic sources. The first class is the heat production in Earth’s interior that generates forces known in geology as internal or endogenous. The internal forces drive all the vertical and horizontal movements of Earth’s crust and are responsible for some severe disasters such as earthquakes or volcanic eruptions. The second class—the external or exogenous forces—is generated by energetic input from the Sun. They trigger motions in Earth’s hydrosphere and atmosphere and tend, through weathering, erosion, and sedimentation, to decrease the morphological expressiveness created by internal forces. This is an expression of the second theorem of thermodynamics predicting dissipative exchange of energy between systems that are in mutual disequilibrium. Generally, if there were no atmosphere and hydrosphere on Earth, the internal forces would produce extremely rugged surface morphology with any kind of steep positive or negative forms that could sustain gravitational forces. On the other hand, if there were no internal forces, erosion would quickly diminish all morphological variations and Earth would become a boringly flat spheroid body. The purpose of this article is to outline how the internal forces are generated, distributed, and dissipated, and how they influence the composition, structure, movements, and deformation within the upper layers of the solid Earth. 2. The Earth’s Interior—Thermal and Compositional Structure UNESCO – EOLSS 2.1. Internal Heat The degree of surface instability of every planet in the Solar System is proportional to its internal mobilitySAMPLE (i.e., to the ability of masses CHAPTERS in the planetary interiors to move due to accommodation of thermal and gravitational instabilities). This can be expressed by the ratio of volume (V) to the surface area (S) as being proportional to radius (R) in the equation: V 4 π R 3 R = 3 = S 4π R 2 3 This means that this ratio is high for large planets and they cool slowly due to their smaller surface area per volume compared to small planets and moons, which have a ©Encyclopedia of Life Support Systems (EOLSS) EARTH SYSTEM: HISTORY AND NATURAL VARIABILITY – Vol. I - Internal Forces and Their Influence on the Earth’s Surface - Plašienka D. comparatively low heat capacity and a large surface area per volume to cool out. Accordingly, large planets are hot and mobile, depending on their compositions. Among the terrestrial planets composed mostly of silicates, only those with large radii are able to store enough thermal energy to reduce the strength of rock masses in their interiors. Increasing temperature lowers the rock strength exponentially and every rock begins to flow at a certain temperature. This holds for Earth and Venus in particular, which are hot enough for their interiors to be highly mobile. In the case of Earth, the internal thermal and, consequently, gravitational instabilities vanish due to mass movements that are transferred towards the surface and expressed by various kinds of deformation and movements of the upper, seemingly stiff layers of Earth. Accordingly, Earth may be regarded as a heat engine, though Earth’s internal thermal input power is rather low (approximately 1 × 107 MW, which is comparable to the energetic production of the whole of humankind). The principal sources of internal heat are considered to be twofold: (1) the heat inherited from the early accretionary period of Earth and (2) the radiogenic heat produced by decay of radioactive elements presently involved in Earth’s crust and mantle. During the earliest stages of Earth’s history (some 4.7–4.5 billion years ago), its internal heat rose gradually, being generated by transformation of the kinetic energy of incident particles forming the early Earth and by the thermal energy released during the gravitational collapse, adiabatic compression and an increase of the density of Earth’s body. Later on, the temperature in Earth’s interiors reached the melting point, which enabled the gravitational differentiation of rock masses producing additional heat. However, the radiogenic heat production has been the most important input power during the whole of Earth’s history. It is generated by the breakdown of radioactive isotopes, which had originally been randomly distributed within the early Earth’s body but, being comparatively light, became concentrated in Earth’s upper layers after the gravitational differentiation. (See Early Earth). Earth’s body is thermally inhomogeneous. The temperature in its core reaches 6000 °C, while the surface temperature approaches 0 °C. Obviously the temperature increases with depth. This downward increase (directed to Earth’s center) is known as the geothermal gradient, a measure of rise in temperature per unit length. Surface and subsurface measurements in deep wells and mines indicate this gradient to be in the range of 10–40UNESCO °C km–1, most typically 20–25 – °CEOLSS km–1. However, an extrapolation of this value to Earth’s interiors would mean unrealistically high temperatures, therefore the thermal gradient has to decrease with depth. This is in line with the observation that the radioactive elements as the main sources of Earth’s heat production are concentrated in the crust. Nevertheless,SAMPLE Earth is hottest in itsCHAPTERS center and coldest on its surface, which indicates that a great deal of its thermal energy is being dissipated on the surface. In fact, this and other losses only slightly exceed the internal heat production, which means that the Earth as a whole cools very slowly, negligibly with respect to the length of human existence. Variations in the near-surface geothermal gradient are an expression of a changing heat flow, a measure of the thermal input from Earth’s interiors towards its surface. The heat flow density indicates the amount of heat that is released from Earth’s surface per unit area and per unit time. Within Earth’s body, the heat is transported in two principal ©Encyclopedia of Life Support Systems (EOLSS) EARTH SYSTEM: HISTORY AND NATURAL VARIABILITY – Vol. I - Internal Forces and Their Influence on the Earth’s Surface - Plašienka D. ways—by conduction and convection. Thermal conduction differs for various rocks, and prevails in the stiff upper layers of Earth. Thermal convection means heat transport by moving matter, and prevails in Earth’s interior. However, many large positive heat flow anomalies on Earth’s surface are dominantly produced by thermal convection, for example by ascending magmatic melts or aqueous and other fluids in active volcanic areas. But also in nonvolcanic areas with thinned crust, which are usually overlain by large and deep sedimentary basins, the heat primarily conveyed from the depths by conduction is then distributed by meteoric waters circulating within the upper crustal rocks. Geothermal energy might be, thanks to its apparent inexhaustibility, one of the most important energy sources for humankind in the future. Nowadays, this energy is only widely utilized in certain areas with high heat flow, to produce electric power and to heat various objects such as buildings or greenhouses. However, the energetic potential of areas with normal and even with lowered heat flow is considerable as well.
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